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ADVERTISEMENT RETURN TO ISSUEPREVCommunicationNEXTReversible 1,2-Migration of Hydrogen between Platinum and Silicon via Intermediate Silylene ComplexesGregory P. Mitchell and T. Don TilleyView Author Information Department of Chemistry University of California at Berkeley Berkeley, California 94720-1460 Cite this: J. Am. Chem. Soc. 1998, 120, 30, 7635–7636Publication Date (Web):July 17, 1998Publication History Received13 March 1998Published online17 July 1998Published inissue 1 August 1998https://pubs.acs.org/doi/10.1021/ja9808346https://doi.org/10.1021/ja9808346rapid-communicationACS PublicationsCopyright © 1998 American Chemical SocietyRequest reuse permissionsArticle Views443Altmetric-Citations48LEARN ABOUT THESE METRICSArticle Views are the COUNTER-compliant sum of full text article downloads since November 2008 (both PDF and HTML) across all institutions and individuals. These metrics are regularly updated to reflect usage leading up to the last few days.Citations are the number of other articles citing this article, calculated by Crossref and updated daily. Find more information about Crossref citation counts.The Altmetric Attention Score is a quantitative measure of the attention that a research article has received online. Clicking on the donut icon will load a page at altmetric.com with additional details about the score and the social media presence for the given article. Find more information on the Altmetric Attention Score and how the score is calculated. Share Add toView InAdd Full Text with ReferenceAdd Description ExportRISCitationCitation and abstractCitation and referencesMore Options Share onFacebookTwitterWechatLinked InRedditEmail Other access optionsGet e-AlertscloseSupporting Info (1)»Supporting Information Supporting Information SUBJECTS:Anions,Genetics,Hydrogen,Platinum,Silicon Get e-Alerts
Abstract Flux footprints for neutral shear-driven canopy flows are evaluated using large-eddy simulation (LES) and a Lagrangian stochastic (LS) model. The Lagrangian stochastic model is driven by flow statistics derived from the large-eddy simulation. LES results suggest that both surface and elevated sources inside the canopy contribute equally to the cumulative flux from an upwind distance of 4 times the canopy height. LES flux footprints are more contracted than those obtained using the Lagrangian stochastic model. This is attributed to an enhanced vertical diffusion and reduced horizontal diffusion. The ejection and sweep contributions to momentum exchange in the Lagrangian stochastic model are weaker than those in the large-eddy simulation. Ejections of low-momentum air dominate at all levels in the canopy modeled by the LES. In contrast, high-momentum sweep events are dominant within the LES canopy and low-momentum ejection events are dominant above the canopy. Dispersion parameters for the first- and second-order statistics of concentration from both LES and LS for three line sources representing the canopy crown, midcanopy, and surface sources are also investigated. Lagrangian model results are sensitive to the choice of the time scale. A time scale based on the dissipation rate agrees well with the LS and LES plume heights of surface source. However, flux footprints from LS are closer to those from the LES, while an intermediate time scale (0.15z/σw) was used inside the canopy.
Allylic substitution catalyzed by copper261- 269 is a transformation that is related to allylie substitutions catalyzed by other transition metals discussed previously in this chapter, but several features of copper-catalyzed allylations make them worth differentiating. First, copper-catalyzed allylic substitutions are conducted with different types of nucleophiles than most allylic substitutions catalyzed by other metals. Second, the regioselectivity of the copper-catalyzed reactions is typically different from that of reactions catalyzed by complexes of other metals, particularly of reactions catalyzed by complexes of palladium. Thus, this last section of the chapter describes studies on allylic substitution catalyzed by copper, with an emphasis on enantioselective examples.
A study of charge cycling at the Li/poly[bis(2,3‐di‐(2‐methoxyethoxy)propoxy)phosphazene] interface is reported. Irreversible processes occurring at the Li/solid polymer electrolyte interface have been characterized by using high‐sensitivity dilatometry and electrochemical impedance spectroscopy (EIS) as a function of cycle number. The volume of a Li/solid polymer electrolyte/Li laminate initially increases with cycle number but then attains a steady state after approximately 450 cycles. The impedance, however, is found to remain essentially constant throughout the entire cycling regime and to be essentially resistive (nonreactive) at frequencies below 10 kHz. A point defect model has been developed to interpret the mechanism of the interfacial charge‐transfer processes in terms of the interstitial transfer of through a corrosion product layer that forms on the metal surface.
An algorithm for modeling the step response behavior of ground stable nonlinear devices and systems is presented. The algorithm converges in the mean-square sense to an exact orthogonal representation whenever the nonconstant component of the step response is a finiteenergy signal. Terminating the algorithm after <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">N</tex> iterations results in an <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">N</tex> th-order model whose dynamics are segregated from the nonlinearity in the tradition of Wiener. The model admits a simple circuit realization, and the parameters which characterize it. <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">N + I</tex> nonlinear functions of a single variable, can all be obtained directly from terminal measurements. Three examples are cited, and a class of nonlinear differential systems is identified for which the algorithm converges.